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This study quantifies the necessity of retaining higher irreducible representation states when simulating SU(3) lattice gauge theory in weak-coupling regimes using quantum computers. By measuring relative probabilities via Euclidean Monte Carlo and perturbation theory, the authors provide critical data for optimizing truncation schemes that balance computational efficiency with physical accuracy. These findings directly inform the design of qubit mappings for continuous gauge groups, addressing a fundamental bottleneck in scalable quantum simulations of QCD.
Impact of Irrep Truncations on Quantum Simulations of QCD
arXiv:2610.23681v1 Announce Type: cross Abstract: Quantum simulations of lattice gauge theories with continuous gauge groups require a choice of basis (how states of the gauge theory map to the qubit computational basis) and truncation scheme (which of the infinitely many gauge theory basis states should be omitted in the map to the finite dimensional qubit Hilbert space.) The most common choices are adapted to an electric basis for the gauge theory, where the basis states for each link are associated with irreducible representations of the gauge group. Electric bases and truncations are generally advantageous for preserving gauge symmetries and simulating the strong coupling regime, but their effectiveness in the weak coupling regimes of physical interest are less well understood. In this work, we compute relative probabilities $p(R')/p(R)$ for finding a link in the irreps $R,R'$ in the ground state of SU(3) lattice gauge theory using Euclidean Monte Carlo methods and weak-coupling lattice perturbation theory. The observables that compute these relative probabilities are constructed by introducing seams into an anisotropic lattice, and by a similar construction we are also able to measure relative probabilities of different site singlets (ways that electric flux braids together into a gauge singlet) at each vertex. With these methods we can quantify, for example, the importance of higher electric flux states in the weak coupling ground state. These results directly inform what truncations are needed to accurately capture non-abelian gauge dynamics near the continuum limit.
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